Geometrical and Electronic Structures of Gold, Silver, and Gold−Silver

In a neutral alloy, the equivalent mixing is favored, and the even numbered k tends ... View: PDF | PDF w/ Links | Full Text HTML ... For a more compr...
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J. Phys. Chem. B 2003, 107, 9994-10005

Geometrical and Electronic Structures of Gold, Silver, and Gold-Silver Binary Clusters: Origins of Ductility of Gold and Gold-Silver Alloy Formation Han Myoung Lee, Maofa Ge, B. R. Sahu, P. Tarakeshwar, and Kwang S. Kim* National CreatiVe Research InitiatiVe Center for Superfunctional Materials, Department of Chemistry, DiVision of Molecular and Life Sciences, Pohang UniVersity of Science and Technology, San 31, Hyojadong, Pohang 790-794, Korea ReceiVed: March 31, 2003; In Final Form: June 10, 2003

The structures of pure gold and silver clusters (Auk, Agk, k ) 1-13) and neutral and anionic gold-silver binary clusters (AumAgn, 2 e k ) m + n e 7) have been investigated by using density functional theory (DFT) with generalized gradient approximation (GGA) and high level ab initio calculations including coupled cluster theory with relativistic ab initio pseudopotentials. Pure Auk clusters favor 2-D planar configurations, while pure Agk clusters favor 3-D structures. In the case of Au, the valence orbital energies of 5d are close to that of 6s. This allows the hybridization of 6s and 5d orbitals in favor of planar structures of Auk clusters. Even 1-D linear structures show reasonable stability as local minima (or as global minima in a few small anionic clusters). This explains the ductility of gold. On the other hand, the Ag-4d orbital has a much lower energy than the 5s. This prevents hybridization, and so the coordination number (Nc) of Ag in Agk tends to be large in s-like spherical 3-D coordination in contrast to that of Au in Auk which tends to be small in 1-D or 2-D coordination. This trend is critical in determining the cluster structures. The calculated electronic properties and dissociation energy of both pure and binary clusters are in good agreement with the available experimental data. Since the Ag-5s orbital is much higher in energy than the Au-6s orbital energy, the partial charge transfer from Au to Ag takes place in gold-silver binary clusters. Au atoms tend to be negatively charged, while Ag atoms tend to be positively charged. Combined with the trend that Au atoms favor the surface, edges, or vertices with smaller Nc, the outer part of the cluster tends to be negatively charged, while Ag atoms favor the inside with larger Nc, and so the inner part tends to be positively charged. The partial charge transfer in the binary system results in electrostatic energy gain for the binary AumAgn cluster over pure Auk and Agk clusters, which is responsible for the formation of alloys. In a neutral alloy, the equivalent mixing is favored, and the even numbered k tends to be more stable due to the electron spin pairing, whereas in an anionic alloy the odd numbered k tends to be more stable.

1. Introduction The intense quest toward the design of novel nanofunctional materials (such as quantum dot, nanoclusters, and nanowires) has motivated several studies on small-sized metallic clusters (either with or without interaction with ligands).1-4 The goal of most of these studies is to examine the modulation of the physical properties as a result of a decrease in the size. The dominance of quantum effects in such small dimensions leads to the emergence of several interesting characteristics. Bimetallic clusters, in particular, have drawn considerable attention in recent years due to their unique electronic, magnetic, optical, and mechanical properties. For example, a new class of highly efficient optical materials based on AumAgn clusters (to be denoted as “m.n”), having vastly enhanced optical nonlinearity over the bulk metals, have recently been synthesized.5,6 They are considered to be a promising class of catalysts that exhibit superior properties compared to pure metals, in terms of activity, selectivity, stability, and resistance to poisoning.7 Gold-silver clusters and nanoparticles play an important role in catalysis, colloidal chemistry, and medical science.8 New molecular nanocrystalline materials with gold and silver nanoclusters and nanowires, which would be considered as prototypes * Corresponding author phone: 82-54-279-2110; fax: 82-54-279-8137, 3399; e-mail: [email protected].

for electronic nanodevices and biosensors, have also been synthesized.9 Although much of the experimental and theoretical work so far has been done on pure gold and silver clusters and nanoparticles,10-25 much less is known about the geometrical structures and energetics of binary clusters. These nanoclusters are expected to exhibit interesting electronic and spectral properties, which dramatically change with their sizes. On the experimental side, there are reports on the measurement of dissociation energy (D0) of AuAg using resonant two-photon ionization spectroscopy.13 An anion photoelectron spectroscopy (PES) study on AumAgn (2 e k ) m + n e 4) clusters is available only recently.14 In a while, the structures of gold and silver clusters have been theoretically investigated by a few research groups. Koutecky and co-workers20 did a detailed study of structural isomers of small neutral and anionic silver clusters up to nonamer by using Hartree-Fock and correlated ab initio methods. Fournier21 studied the silver clusters at the levels of DFT (VWN), sum of square-roots of atomic coordinations (SSAC), and extended Hu¨ckel molecular orbital (EHMO) theory. Gronbeck and Andreoni22 used 11 e- pseudopotential and studied the groundstate structures of gold clusters with Becke-Lee-Yang-Parr (BLYP) exchange-correlation functionals. Landman and co-

10.1021/jp034826+ CCC: $25.00 © 2003 American Chemical Society Published on Web 08/26/2003

Gold and Gold-Silver Alloy Formation

J. Phys. Chem. B, Vol. 107, No. 37, 2003 9995

TABLE 1: Comparison of Calculated and Experimental Adiabatic Ionization Potentials (IPa in eV), Vertical Detachment Energies (VDE in eV) [or Electron Affinities (EA in eV) in Brackets], Dissociation Energies (D0 or 2D0* in eV), and Bond Lengths (r in Å in the Dimer) of Neutral and Anionic Au, Ag, Au2, AuAg, and Ag2a IPa

AumAgn (m.n) Au Ag Au2 AuAg Ag2 Au2AuAgAg2-

(1.0) (0.1) (2.0) (1.1) (0.2) (2.0) (1.1) (0.2)

BPW EC (SDB) 9.52(9.56) 7.91(8.04) 9.32(9.38) 8.61(9.71) 7.83(7.97)

MP2 EC (SDB)

D0 (neutral), D0′ (anion)

VDE [EA]

expt

8.39(9.23) 9.23 6.76(7.47) 7.57 8.60(9.59) 9.20 ( 0.21 7.62(8.64)